GB2562278A - Test apparatus - Google Patents

Test apparatus Download PDF

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Publication number
GB2562278A
GB2562278A GB1707517.7A GB201707517A GB2562278A GB 2562278 A GB2562278 A GB 2562278A GB 201707517 A GB201707517 A GB 201707517A GB 2562278 A GB2562278 A GB 2562278A
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United Kingdom
Prior art keywords
magnetic
current sensor
electrical current
flexible
sensor according
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Granted
Application number
GB1707517.7A
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GB2562278B (en
GB201707517D0 (en
Inventor
Zurek Stanislaw
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Megger Instruments Ltd
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Megger Instruments Ltd
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Priority to GB1707517.7A priority Critical patent/GB2562278B/en
Publication of GB201707517D0 publication Critical patent/GB201707517D0/en
Priority to PCT/GB2018/051252 priority patent/WO2018206953A1/en
Priority to SI201830249T priority patent/SI3635415T1/en
Priority to ES18732406T priority patent/ES2864001T3/en
Priority to EP18732406.6A priority patent/EP3635415B1/en
Priority to PL18732406T priority patent/PL3635415T3/en
Publication of GB2562278A publication Critical patent/GB2562278A/en
Application granted granted Critical
Publication of GB2562278B publication Critical patent/GB2562278B/en
Priority to US16/676,843 priority patent/US11009537B2/en
Active legal-status Critical Current
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R27/00Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom
    • G01R27/02Measuring real or complex resistance, reactance, impedance, or other two-pole characteristics derived therefrom, e.g. time constant
    • G01R27/26Measuring inductance or capacitance; Measuring quality factor, e.g. by using the resonance method; Measuring loss factor; Measuring dielectric constants ; Measuring impedance or related variables
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R15/00Details of measuring arrangements of the types provided for in groups G01R17/00 - G01R29/00, G01R33/00 - G01R33/26 or G01R35/00
    • G01R15/14Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks
    • G01R15/18Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using inductive devices, e.g. transformers
    • G01R15/183Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using inductive devices, e.g. transformers using transformers with a magnetic core
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R15/00Details of measuring arrangements of the types provided for in groups G01R17/00 - G01R29/00, G01R33/00 - G01R33/26 or G01R35/00
    • G01R15/14Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks
    • G01R15/18Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using inductive devices, e.g. transformers
    • G01R15/186Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using inductive devices, e.g. transformers using current transformers with a core consisting of two or more parts, e.g. clamp-on type
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R19/00Arrangements for measuring currents or voltages or for indicating presence or sign thereof
    • G01R19/0092Arrangements for measuring currents or voltages or for indicating presence or sign thereof measuring current only
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R27/00Arrangements for measuring resistance, reactance, impedance, or electric characteristics derived therefrom
    • G01R27/02Measuring real or complex resistance, reactance, impedance, or other two-pole characteristics derived therefrom, e.g. time constant
    • G01R27/08Measuring resistance by measuring both voltage and current

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)

Abstract

A flexible electrical current sensor 1 comprising a solenoid 2 disposed about an at least partially magnetic core 3. The core comprises at least one magnetic element 4. The at least one magnetic element having one or more regions of overlap 5 such that a gap is provided in each region of overlap. Each respective gap is configured such that the effective magnetic permeability of the core is maintained during flexing. The gap may maintain a substantially constant volume of the region of overlap. The core may comprise a plurality of magnetic elements in at least one layer on a flexible non-magnetic substrate (6, Fig. 3). The ratio of between the average distance between the layers and the average between elements in first and second layers of elements may be maintained during flexing. The magnetic elements may be arranged to pivot about a point (9, Fig. 4) in a region of overlap. There may be one magnetic element arranged helically. There may be two magnetic elements arranged as intertwining strips.

Description

FLEXIBLE CURRENT SENSOR
Technical Field
The present invention relates to a flexible electrical current sensor, in particular a flexible electrical current sensor with a solenoid disposed about an at least partially magnetic core having an effective magnetic permeability that is maintained during flexing.
Background
Flexible current sensors, in the form of a Rogowski coil (herein “RC”), have been known since the end of the 19th century and are commonly used today for measuring electrical currents. Modern versions typically have a non-magnetic core, for example made from silicon rubber or plastic. F. Alves, “High-frequency behaviour of magnetic composites based on FeSiBCuNb particles for power electronics”, IEEE Trans. Magnetics, Vol. 38 (5), 2002, p. 3135 describes a structure with magnetic flakes dispersed in a non-magnetic matrix.
Ren, Shiyan, Jiang Cao, and Huayun Yang. "Research of a novel Rogowski coil with special magnetic core." Precision Electromagnetic Measurements Digest, 2008. CPEM2008. Conference on. IEEE, 2008 describes a Rogowski coil with a core having embedded particles.
Summary
According to an aspect of the present invention, there is provided a flexible electrical current sensor comprising a solenoid disposed about an at least partially magnetic core, the at least partially magnetic core comprising at least one magnetic element, wherein the at least one magnetic element is configured to provide one or more regions of overlap such that a respective gap is provided in each region of overlap, each respective gap being configured such that the effective magnetic permeability of the at least partially magnetic core is maintained during flexing.
This allows the core, and the flexible current sensor as a whole, to have an effective magnetic permeability that is controllable at the design stage, by the design of the positioning and overlap of the at least one magnetic element, and that is maintained during flexing of the flexible current sensor. The effective magnetic permeability of the present flexible current sensor may therefore have greater controllability and predictability than known current sensors, while flexibility of the current sensor allows it to be useful in a wide range of applications involving measurement of electrical current.
In some embodiments of the invention, each respective gap is configured to maintain a substantially constant volume of the respective region of overlap provided by the at least one magnetic element.
In some embodiments of the invention, the at least partially magnetic core comprises a plurality of magnetic elements, and the magnetic elements are arranged in at least one layer disposed on a flexible non-magnetic substrate. This allows the core, and the current sensor as a whole, to be flexible while having an effective magnetic permeability that is controllable by the positioning of the magnetic elements on the nonmagnetic substrate.
In some embodiments of the invention, the at least partially magnetic core comprises a first layer of magnetic elements disposed on a first side of the flexible nonmagnetic substrate, and further comprises a second layer of magnetic elements disposed on an opposite side to the first side of the flexible non-magnetic substrate. This allows the spacing, and thus magnetic coupling, between magnetic elements in the same and/or adjacent layer to be controllable. The effective magnetic permeability may therefore be set by the positioning of the magnetic elements, and maintained during flexing of the at least partially magnetic core.
In some embodiments of the invention, a ratio g/o of the average distance between the first and second layers of magnetic elements g, and the average overlap between magnetic elements in the first and second layers o, is maintained during flexing.
In some embodiments of the invention, the at least partially magnetic core comprises a plurality of magnetic elements and the magnetic elements are arranged in at least two layers such that each magnetic element in a layer overlaps with a magnetic element in an adjacent layer. Each magnetic element is arranged to pivot about a point in a region of overlap with another magnetic element. Pivoting of the magnetic elements relative to one another allows the current sensor to be flexible, while the spacing of the layers, and of the magnetic elements within the layers, allows the effective magnetic permeability of the at least partially magnetic core to be controllable.
In some embodiments of the invention, the flexible electrical current sensor comprises one magnetic element arranged substantially helically. In other embodiments of the invention, the flexible electrical current sensor comprises two magnetic elements arranged as intertwining strips.
In some embodiments of the invention, the solenoid comprises winding of a uniform pitch. This allows the current sensor to be more accurate, i.e. improves measurement uncertainty, due to the relationship between the current being measured and the output voltage.
In some embodiments of the invention, the magnetic element(s) have a relative magnetic permeability of at least 500. In some embodiments, the magnetic element(s) comprise magnetically soft material.
Further features and advantages of the invention will become apparent from the following description of preferred embodiments of the invention, given by way of example only, which is made with reference to the accompanying drawings.
Brief Description of the Drawings
The invention will now be described, by way of example only, with reference to the accompanying drawings, in which:
Figure lisa schematic diagram of a perspective view of a flexible current sensor according to embodiments of the invention;
Figure 2 is a schematic diagram of a perspective view of a flexible current sensor according to embodiments of the invention;
Figure 3 is a schematic diagram of a perspective view of a flexible current sensor according to embodiments of the invention;
Figure 4a is a schematic diagram of a side-on view of a flexible current sensor according to embodiments of the invention;
Figure 4b is a schematic diagram of a top-down view of the flexible current sensor shown in Figure 4a;
Figure 5 is a schematic diagram of a perspective view of a flexible current sensor according to embodiments of the invention;
Figure 6 is a schematic diagram of a top-down view of a flexible current sensor according to embodiments of the invention;
Figure 7 is a schematic diagram of a perspective view of an at least partly magnetic core for a flexible current sensor according to embodiments of the invention;
Figure 8 is a schematic diagram of a top-down view of an at least partly magnetic core for a flexible current sensor according to embodiments of the invention;
Figure 9a is a schematic diagram of a perspective view of a test apparatus comprising a flexible current sensor according to embodiments of the invention;
Figure 9b is a schematic diagram of a perspective view of the test apparatus shown in Figure 9a in a different configuration; and
Figure 10 is a schematic diagram of a perspective view of a test apparatus comprising a flexible current sensor according to embodiments of the invention.
Detailed Description
Embodiments of the invention are herein described with reference to the accompanying drawings. In the following description, for the purpose of explanation, numerous specific details of certain examples are set forth. Reference in the specification to "an example" or similar language means that a particular feature, structure, or characteristic described in connection with the example is included in at least that one example, but not necessarily in other examples. It should further be noted that certain examples are described schematically with certain features omitted and/or necessarily simplified for ease of explanation and understanding of the concepts underlying the examples.
Rogowski coils (RCs) are used mainly for measuring alternating currents (AC). They may provide reliable performance and linearity at currents of kilo-amperes (kA), in a wide frequency range up to megahertz (MHz). However, the non-magnetic core means that their sensitivity is relatively low and they typically cannot measure accurately below 1 ampere (A). For normal RC construction, 10 milli-amperes (mA) may be the lowest current measurable. Generally, the term “Rogowski coil” implies a sensor with a non-magnetic core. However, sensors with magnetic (or partially magnetic) cores may also be referred to as Rogowski coils.
The operation of Rogowski coils and the present flexible current sensor is based on a relationship between an input current passing through, and being measured by, the coil and a generated output voltage. With the relationship known, the output voltage can be measured and the input current inferred. This relationship may be given by:
where Lout is the output voltage, d/in(Z)/dZ is the time differential of the input current as a function of time /m(Z), μχ is the relative magnetic permeability of the medium, /zo is the magnetic constant or magnetic permeability of vacuum, A is the cross-sectional area of the core about which turns of wire are wound, I is the magnetic path length, and the sum is over each turn z up to the total number of turns N. The sum of partial voltages, each partial voltage corresponding to the voltage through each turn z of the coil, may also be referred to as a space integral.
For better proportionality between the output voltage Lout and input current /m(z), the other terms in the equation should be kept as constant as possible throughout the core of the current sensor, /zo is a natural constant, while A and I are relatively straightforward to manufacture such that they are constant throughout the coil. Thus, a current sensor where /zt is constant and the spacing between the turns of the coil is constant (uniform winding) would improve the measurement accuracy of a current.
The relative magnetic permeability of a material is related to a magnetic field strength H (measured in amps per metre) and a magnetic flux density B (measured in tesla) by B = /zo /zr H. Thus, a constant μχ gives a linear relationship between B and H.
Introducing an air gap into a magnetic core may reduce the magnetic permeability μχ of the core while also increasing the linearity of the relationship between the magnetic field strength H and magnetic flux density B - sometimes referred to as a B-H curve or loop. The effective magnetic permeability /zeff of such a magnetic core with a gap may be considered to be:
where //core is the magnetic permeability of the core material, /core is the length of the core, and /gap is the length of the air gap. This equation is based on several assumptions, such as: the cross section area of the magnetic circuit is constant at every point of the circuit, and is the same for the core and for the gap; the length of the air gap is much shorter than the total path length of the magnetic core; the magnetisation is uniform and fringing effect is neglected; and the permeability of the core material is much greater than the permeability of air gap.
It is an object of the present invention to provide a current sensor that is flexible and has increased uniformity of effective magnetic permeability, even during flexing, such that measurements of low current (for example, current below 1 A) may be made with a higher value of certainty than known current sensors. For example, in current sensors where magnetic powder, particles or flakes is/are dispersed in a non-magnetic matrix or substrate, it may be difficult to determine with sufficient accuracy the number of such particles present in a given volume of material. The uniformity of such a structure must therefore be estimated by statistical averaging. In the present flexible current sensor, however, the uniformity of the structure is controlled by mechanical properties, and so may be determined and controlled to greater accuracy. The effective magnetic permeability of the present flexible current sensor may therefore have greater controllability and predictability.
Figures 1 to 6 show a flexible electrical current sensor 1 comprising a solenoid 2 disposed about an at least partially magnetic core 3. The at least partially magnetic core 3 comprises at least one magnetic element 4. The at least partially magnetic core 3 may, in some examples, comprise magnetic and non-magnetic parts and hence is referred to as at least partially magnetic. The at least partially magnetic core 3 may significantly increase sensitivity of the present current sensor compared to Rogowski Coils with non-magnetic cores, for example by a factor of around 30 to 50 times, or even exceeding 250 times for small currents.
The at least one magnetic element 4 is configured to provide one or more regions of overlap 5 such that a respective gap is provided in each region of overlap 5. A region of overlap may be a spatial region where at least two portions of a magnetic element 4, or at least two magnetic elements 4, overlap each other. The respective gap of each region of overlap 5 may be a geometrical function of a length of overlap, and a distance between the at least two portions of a magnetic element 4, or at least two magnetic elements 4, for example.
Compared with current sensors having a core comprising magnetic particles or flakes dispersed in a non-magnetic matrix, the positioning of the discrete magnetic element(s) 4 in the present flexible current sensor 1 may be controlled to greater precision. Thus, instead of an inhomogeneous distribution of magnetic particles, giving varying magnetic couplings between each pair of particles due to their varying non-uniform separations, the magnetic elements 4, or particular parts of a singular magnetic element 4, in the present flexible current sensor 1 may be positioned to a greater accuracy and precision relative to one another. This allows for a greater controllability and predictability of the effective magnetic permeability of the core structure 3.
Each respective gap is configured such that the effective magnetic permeability of the at least partially magnetic core 3 is maintained during flexing. In some examples, the effective magnetic permeability of the at least partially magnetic core 3 is much greater than 1, for example at least 500, which may improve the sensitivity of the flexible electrical current sensor 1 allowing smaller currents, for example 1 mA and below, to be measured. This provides a significant improvement in sensitivity over comparable RCs, with high-sensitivity RCs measuring currents in the order of 10 mA. In an example, the effective magnetic permeability of the at least partially magnetic core 3 is at least 2. In other examples, the effective magnetic permeability of the at least partially magnetic core 3 is approximately 30, or 100.
In certain cases, the effective magnetic permeability of the at least partially magnetic 3 core is maintained during flexing to within 1%, 2% 3%, 4%, 5%, or less than 10?zo of an effective magnetic permeability value when the core 3 is at rest or unflexed.
In some embodiments, each respective gap is configured to maintain a substantially constant volume of the respective region of overlap 5 provided by the at least one magnetic element 4. For example, a volume of the respective region of overlap 5 may be delimited by the dimensions of the respective region of overlap 5, such as the overlapping area of the magnetic elements 4, or portions of a magnetic element 4, and a distance between the magnetic elements 4, or portions of a magnetic element 4.
In some embodiments, each respective gap comprises no electronics or electronic components, for example a transducer or sensor. In other words, such electronic components are absent from each respective gap provided in each region of overlap 5, and in particular active electronic components are absent from each respective gap provided in each region of overlap 5.
Figure 2 shows an embodiment where the at least partially magnetic core 3 comprises one magnetic element 4 arranged substantially helically. The magnetic element 4 is configured to provide regions of overlap 5 where the magnetic element 4 overlaps itself in its helical arrangement. The substantially helical arrangement of the magnetic element 4 may in some examples have a substantially circular cross-section, but in other examples have a non-circular cross-section. For example, the cross-section of the helix that the magnetic element 4 traces may be elongated or “flattened”.
Figure 3 shows an embodiment with the at least partially magnetic core 3 comprising a flexible non-magnetic substrate 6. The flexible non-magnetic substrate may be, for example, polycarbonate plastic tape. In some examples of this embodiment, the flexible non-magnetic substrate 6 is between 0.01 and 1.0 mm in thickness. In examples of larger sensors, the flexible non-magnetic substrate 6 may be greater than 10 mm in thickness.
The at least partially magnetic core 3 may comprise a plurality of magnetic elements 4, with the magnetic elements 4 arranged in at least one layer disposed on the flexible non-magnetic substrate 6. The magnetic elements 4 may be affixed to the flexible non-magnetic substrate 6 by an adhesive, for example the flexible nonmagnetic substrate 6 may have an adhesive layer. The magnetic elements 4 may be metallic strips in certain cases.
In the embodiment shown in Figure 3, the at least partially magnetic core 3 comprises a first layer 7 of magnetic elements 4 disposed on a first side of the flexible non-magnetic substrate 6, and a second layer 8 of magnetic elements 4 disposed on an opposite side to the first side of the flexible non-magnetic substrate 6. In other embodiments, the at least partially magnetic core 3 may comprise multiple layers of magnetic elements 4 disposed on opposite sides of the flexible non-magnetic substrate 6. The at least partially magnetic core 3 having two layers 7, 8 as shown in Figure 3 may be beneficial for manufacturing. The relative magnetic permeability μ of the magnetic elements 4 may be greater than 500 or 1000 in some examples, and preferably at least 10,000. The magnetic field is guided along a magnetic element 4, because it is energetically much easier for the field to flow inside of a high-// magnetic element than through the non-magnetic substrate 6. However, the magnetic elements 4 have finite length and so at the end of the element 4, the field is forced to jump across to the next high-// magnetic element via the shortest possible path, which will start and end perpendicularly to the surfaces of adjacent magnetic elements 4.
In another embodiment, the at least partially magnetic core 3 comprises a plurality of magnetic elements 4 arranged in at least one layer 7, 8 and disposed at least partially within the flexible non-magnetic substrate 6. For example, instead of the magnetic elements 4 being disposed on a surface of the flexible non-magnetic substrate 6 as shown in Figure 3, the magnetic elements 4 may be embedded, partially or fully, in the flexible non-magnetic substrate 6. The embedding may be achieved, for example, by over-moulding in rubber or via 3D printing.
In certain cases, the magnetic elements 4 may be skewed at an angle relative to the longitudinal axis of the at least partially magnet core 3, for example the magnetic elements may have a longitudinal axis that is not parallel nor orthogonal to the longitudinal axis of the flexible non-magnetic substrate 6. In these cases, adjacent magnetic elements 4 may overlap one another in a common plane.
In another embodiment, the plurality of magnetic elements 4 are arranged in at least two layers 7, 8, wherein each layer of magnetic elements 7, 8 is disposed at least partially within the flexible non-magnetic substrate 6, such that each magnetic element 4 in a layer 7, 8 overlaps with a magnetic element 4 in an adjacent layer 7, 8.
An effective magnetic permeability //comp of the example composite core 3 shown in Figure 3 may be given by:
where: //mat is the magnetic permeability of the magnetic elements; g is the distance between magnetic elements 4 in different layers 7, 8; t is the thickness of the magnetic elements; o is the length of the overlap region 5, along a longitudinal axis of the core 3, between magnetic elements 4 in different layers 7, 8; and s is the length of the magnetic elements along the longitudinal axis of the core 3. In some examples, the quantities g, t, o, and s may be averaged over the entire core 3. In other examples, the magnetic elements 4 may be uniform and arranged homogeneously along the length of the at least partially magnetic core 3, such that these quantities will have substantially the same value for each magnetic element 4 and each relationship between magnetic elements 4.
The quantity 2g t/o may be considered to be an effective gap length of the at least partially magnetic core 3 comprising two layers 7, 8 of magnetic elements 4 (analogous effective gap length expressions may be specified for partially magnetic cores 3 comprising a different number of layers 7, 8). For example, when comparing the above equation for the effective magnetic permeability //comp of the composite core 3 shown in Figure 3 to the general equation for effective magnetic permeability g«s of a core with a gap, it can be seen that the ratios /gap/^core and 2g ' t/o · s are related. In an at least partially magnetic core 3 made up of multiple uniform elements, each of length e, the length 5 of a magnetic element 4 is related to the total effective length of the magnetic elements 4 in the core 3 by a factor of e. This factor is cancelled out when multiplying the effective gap length for an element (2g t/o) by e.
In some embodiments, the ratio g/o of: the average distance g between the first and second layers 7, 8 of magnetic elements 4; and the average overlap o between magnetic elements 4 in the first and second layers 7, 8; is maintained during flexing of the flexible electrical current sensor 1. For example the ratio g/o may be maintained during flexing to within 10% of a value at rest, in other words when the sensor is unflexed. Thus, by using magnetic elements 4 with uniform thickness t, the effective gap length of the at least partially magnetic core 3, and therefore its effective magnetic permeability //comp, may be kept constant. This allows for the linearity of the relationship between B and H, and between Tout and /in to be maintained throughout the at least partially magnetic core 3, and during flexing of the electrical current sensor 1. The magnetic elements 4 may also have a high relative magnetic permeability of at least 500, 1000 or 10,000. This allows for high sensitivity of the electrical current sensor 1, with measurements of below 1 mA possible, while being flexible so that it can be wrapped around a current-carrying structure, and thus useful in a wide range of applications.
Figures 4a and 4b show an embodiment wherein the magnetic elements 4 are arranged in two layers such that each magnetic element 4 in a layer overlaps with a magnetic element 4 in an adjacent layer. Each magnetic element 4 is arranged to pivot about a point 9 in a region of overlap 5 with another magnetic element 4. Figure 4a shows a side-on view of the sensor 1, while Figure 4b shows a top-down or “birds-eye” view. In some examples, there are more than two layers of magnetic elements 4.
In the embodiment shown in Figures 4a and 4b, there are non-magnetic spacers 10 between overlapping magnetic elements 4, and the non-magnetic spacers 10 are positioned in the regions of overlap 5. Thus, pivoting of the magnetic elements 4 provides the flexibility of the partially magnetic core 3 and electrical current sensor 1 as a whole.
In other embodiments, the magnetic elements 4 may be arranged in more than two layers such that magnetic elements 4 in a layer overlap with magnetic elements 4 in another of the layers.
In other embodiments, the magnetic elements 4 may be arranged in a single layer, for example, a series of magnetic elements 4 connected to one another by nonmagnetic pivots 9.
Figure 5 shows an embodiment where the at least partially magnetic core 3 comprises a plurality of magnetic elements 4 arranged in a single layer and shaped such that adjacent magnetic elements 4 in the single layer overlap. Regions of overlap 5 may be present where adjacent magnetic elements 4 overlap one another due to their shape, for example an ‘S’ or ‘Z’ shape, as shown in Figure 5. Adjacent magnetic elements 4 may be arranged to pivot with respect to one another, for example about a common pivot point in a region of overlap 5.
Figure 6 shows an embodiment where the flexible electrical current sensor 1 comprises two magnetic elements 4 arranged as intertwining strips. The intertwined magnetic elements 4 may have regions of overlap 5 where the strips overlap one another, as shown in Figure 6.
In other embodiments, the magnetic elements 4 may be arranged as rhombic- or parallelogrammatic-shaped strips in one or more layers. In other cases, the strips arranged in one or more layers may be another shape, such as round circles or ovals.
Figure 7 shows an embodiment where the at least partially magnetic core 3 comprises magnetic elements 4a, 4b in a ball-and-socket arrangement. There is a region of overlap 5 where the socket magnetic element 4a covers part of the ball magnetic element 4b, as shown in Figure 7. In some embodiments, the at least partially magnetic core 3 may comprise a series of such magnetic elements 4a, 4b in a ball-and-socket arrangement. In some embodiments, for example, the at least partially magnetic core 3 may comprise a series of magnetic elements, of which at least some comprise a socket end resembling the socket element 4a shown in Figure 7, and a ball end resembling the ball magnetic element 4b shown in Figure 7, such that a ball-and-socket arrangement is provided at each boundary between consecutive magnetic elements.
The ball-and-socket arrangement of the magnetic elements 4a, 4b allows the at least partially magnetic core 3 to flex, as the magnetic elements 4a, 4b may move relative to one another. A flexible electrical current sensor may be formed from a solenoid disposed about the at least partially magnetic core 3 shown in Figure 7, or a series of such magnetic elements 4a, 4b, as in the embodiments shown in the Figures 1 to 6.
Figure 8 shows a top-down view of an embodiment where the at least partially magnetic core 3 comprises one magnetic element 4 arranged in a layer and configured to provide regions of overlap 5 where the magnetic element 4 overlaps itself in the layer. For example, the magnetic element 4 may be meandered as shown in Figure 8 to provide regions of overlap 5 where the magnetic element 4 overlaps itself.
The flexible current sensor 1 according to any of the described embodiments may be elongate for forming a ring or loop around a current-carrying device or structure. In some examples, the magnetic element(s) may be elongate. The longitudinal axis of such elongate magnetic element(s) may be substantially parallel to a longitudinal axis of the at least partially magnetic core and/or the flexible current sensor 1 in an un-flexed rest state.
Figures 9a and 9b show schematically a test apparatus comprising a flexible current sensor 1 according to any of the described embodiments connected to a test unit 11. The test unit 11 may display a measured current value, for example, and may have controls for controlling the test apparatus. The flexible current sensor 1, and where applicable the non-magnetic substrate 6, is sufficiently flexible to allow the flexible current sensor 1 to be opened sufficiently wide and arranged about a current-carrying structure 12 in some embodiments. For example, in the embodiment shown in Figure 9a, the flexible current sensor 1 is flexed to create an opening 13 for the current-carrying structure 12 to be passed through. The flexible current sensor 1 may be flexed to close the opening 13 and form a closed loop, as shown in Figure 9b, for measuring the current passing through the current-carrying structure 12. In other embodiments, the flexible current sensor 1, and where applicable the non-magnetic substrate 6, may be sufficiently flexible to allow the flexible current sensor 1 to be wrapped around the current-carrying structure 12 with multiple turns. In examples, the current-carrying structure 12 may be any conductor for example a wire, a cable, or a metallic structural member such as a support leg of an electricity pylon.
Figure 10 shows schematically a test apparatus comprising the flexible current sensor 1 according to any of the described embodiments connected to the test unit 11. The flexible current sensor comprises a return wire 14 connected to, or as part of, the solenoid 2 which is not shown in the figure. The return wire travels from an end of the solenoid at an end of the flexible current sensor 1 to the other end of the flexible current sensor 1. In this way, the opening 13 may be created by flexing the flexible current sensor 1, with the solenoid 2 and the return wire 14 not obstructing the opening 13, so that the flexible current sensor 1 may be arranged about a current-carrying structure. The return wire connects to the test unit 11 to complete a circuit with the other end of the solenoid 2 being connected to the test unit also.
In some examples, the flexible current sensor 1 may have a releasable joint to open and secure the ends of the flexible current sensor 1 at the opening 13.
In examples, a magnetic element 4 may be a magnetic member, such as a solid piece or strip of material that, as a whole, comprises magnetic properties. In other examples, a magnetic element 4 may be formed by a depression or cavity in the nonmagnetic substrate 6 that is at least partially filled with a magnetic powder or liquid. For example, the concentration of magnetic powder or liquid having a defined boundary with the non-magnetic substrate 6 may be considered a magnetic element 4. A plurality of such cavities in the non-magnetic substrate 6, each at least partially filled with magnetic powder or liquid, may therefore be considered a plurality of magnetic elements 4.
In certain cases, the magnetic element(s) 4 described herein may have a relative magnetic permeability of at least 500, or at least 1,000, or at least 10,000. The magnetic element(s) may comprise magnetically soft material, for example iron (Fe), nickel (Ni), or cobalt (Co), or a mixture comprising at least two of these three metals such as a nickel-iron alloy. In an example, the magnetic elements(s) 4 are made from an alloy comprising 80% nickel and 20% iron. In other cases, the magnetic element(s) 4 may be formed from nanocrystalline or amorphous ribbon, or electrical steel, for example cut into strips. In other examples, the magnetic element(s) may comprise a ferrite, oxide, or powder-based material. In certain cases, the magnetic element(s) may be flexible. In these cases, the magnetic element(s) may flex when the at least partially magnetic core is flexed, with the effective magnetic permeability of the at least partially magnetic core maintained during flexing.
In any of the embodiments and examples described herein, the solenoid 2 disposed about the at least partially magnetic core 3 may have winding of a uniform pitch. As the value for the output voltage depends on a space integral over all turns i of the solenoid 2 up to the total number of turns N, a uniform winding of the solenoid 2 allows the same value for output voltage to be determined regardless of the position of the current sensor with respect to the electrical conductor being measured. Thus, in cases where the solenoid 2 has a winding of a uniform pitch, the present flexible current sensor 1 may be used more reliably, as its position relative to the electrical conductor being measured does not affect the measurement reading.

Claims (18)

1. A flexible electrical current sensor comprising a solenoid disposed about an at least partially magnetic core, the at least partially magnetic core comprising at least one magnetic element, wherein the at least one magnetic element is configured to provide one or more regions of overlap such that a respective gap is provided in each region of overlap, each respective gap being configured such that the effective magnetic permeability of the at least partially magnetic core is maintained during flexing.
2. A flexible electrical current sensor according to claim 1, wherein each respective gap is configured to maintain a substantially constant volume of the respective region of overlap provided by the at least one magnetic element.
3. A flexible electrical current sensor according to claim 1 or 2, the at least partially magnetic core comprising a flexible non-magnetic substrate.
4. A flexible electrical current sensor according to claim 3 wherein the at least partially magnetic core comprises a plurality of magnetic elements, and the magnetic elements are arranged in at least one layer disposed on the flexible nonmagnetic substrate.
5. A flexible electrical current sensor according to claim 4, wherein the layer of magnetic elements is a first layer of magnetic elements disposed on a first side of the flexible non-magnetic substrate, and the at least partially magnetic core further comprises a second layer of magnetic elements disposed on an opposite side to the first side of the flexible non-magnetic substrate.
6. A flexible electrical current sensor according to claim 5, wherein a ratio g/o of the average distance between the first and second layers of magnetic elements g, and the average overlap between magnetic elements in the first and second layers o, is maintained during flexing.
7. A flexible electrical current sensor according to claim 3 wherein the at least partially magnetic core comprises a plurality of magnetic elements, and the magnetic elements are arranged in at least one layer disposed at least partially within the flexible non-magnetic substrate.
8. A flexible electrical current sensor according to claim 3 wherein the at least partially magnetic core comprises a plurality of magnetic elements, and the magnetic elements are arranged in at least two layers, wherein each layer of magnetic elements is disposed at least partially within the flexible non-magnetic substrate, such that each magnetic element in a layer overlaps with a magnetic element in an adjacent layer.
9. A flexible electrical current sensor according to claim 1 or 2, wherein the at least partially magnetic core comprises a plurality of magnetic elements and the magnetic elements are arranged in at least two layers such that each magnetic element in a layer overlaps with a magnetic element in an adjacent layer, and each magnetic element is arranged to pivot about a point in a region of overlap with another magnetic element.
10. A flexible electrical current sensor according to claim 9 comprising nonmagnetic spacers between overlapping magnetic elements, wherein the non-magnetic spacers are positioned in the regions of overlap.
11. A flexible electrical current sensor according to claim 1 or 2, comprising a plurality of magnetic elements arranged in a single layer and shaped such that adjacent magnetic elements in the single layer overlap.
12. A flexible electrical current sensor according to claim 1 or 2, comprising one magnetic element arranged substantially helically.
13. A flexible electrical current sensor according to claim 1 or 2, comprising two magnetic elements arranged as intertwining strips.
14. A flexible electrical current sensor according to any preceding claim, wherein the solenoid comprises winding of a uniform pitch.
15. A flexible electrical current sensor according to any preceding claim, the at least one magnetic element having a relative magnetic permeability of at least 500.
16. A flexible electrical current sensor according to claim 15, the at least one magnetic element having a relative magnetic permeability of at least 10,000.
17. A flexible electrical current sensor according to any preceding claim, wherein the at least one magnetic element comprises magnetically soft material.
18. A flexible electrical current sensor according to claim 17, wherein the at least one magnetic element comprises a ferrite, electrical steel, nickel-iron alloy, or a nanocrystalline or amorphous ribbon.
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PCT/GB2018/051252 WO2018206953A1 (en) 2017-05-10 2018-05-10 Flexible current sensor
SI201830249T SI3635415T1 (en) 2017-05-10 2018-05-10 Flexible current sensor
ES18732406T ES2864001T3 (en) 2017-05-10 2018-05-10 Flexible current sensor
EP18732406.6A EP3635415B1 (en) 2017-05-10 2018-05-10 Flexible current sensor
PL18732406T PL3635415T3 (en) 2017-05-10 2018-05-10 Flexible current sensor
US16/676,843 US11009537B2 (en) 2017-05-10 2019-11-07 Flexible current sensor

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GB2562278B (en) 2019-06-05
US20200072883A1 (en) 2020-03-05
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EP3635415B1 (en) 2021-03-10
SI3635415T1 (en) 2021-07-30

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